不连续相位转换的动态签名:相位共存如何决定指数式与功率定律缩放
Krzysztof Ptaszyński1,2, Massimiliano Esposito1
1Complex Systems and Statistical Mechanics, Department of Physics and Materials Science, <a href="https://ror.org/036x5ad56">University of Luxembourg</a>, L-1511 Luxembourg, Luxembourg.
Physical review. E
|November 20, 2024
概括
这项研究使用大偏差理论阐明了不连续的相位过渡,区分了相位共存 (指数缩放) 和动态性质的无限吸引力 (功率定律缩放).
科学领域:
- 统计力学 统计力学
- 非平衡的物理 物理学
背景情况:
- 关于Liouvillian差距的有限尺寸缩放和不连续相位过渡的动态波动,存在相互矛盾的文献报告.
- 之前的研究表明指数或权力法行为,导致理解这些关键现象的模糊性.
研究的目的:
- 解决文献中关于在不连续相位过渡中有限大小缩放行为的差异.
- 根据它们的动态性质,区分不同类别的不连续相变.
主要方法:
- 应用大偏差理论来分析Liouvillian差距和动态波动.
- 根据系统动态,不连续的相位转换被分为两个不同的类别.
主要成果:
- 确定了两种类型的不连续相变,具有不同的动态特性.
- 第1类 (相共存) 由于吸引子之间的随机切换而呈指数级扩展.
- 2类 (过渡时的无限吸引子) 显示与扩散放松相关的功率定律缩放.
结论:
- 大偏差理论提供了一个框架,以区分不连续相变的动态缩放行为.
- 阶段共存的存在或不存在是决定指数式与权力规律缩放的关键因素.
- 了解这些独特的缩放行为对于描述非平衡相位过渡至关重要.
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